<xml>
  <records>
    <record>
       <contributors>
          <authors>
             <author>Smirnov, V.L.</author>
             <author>Vorozhtsov, S.B.</author>
          </authors>
       </contributors>
       <titles>
          <title>
             A Coupled Cyclotron Solution for Carbon Ions Acceleration
          </title>
       </titles>
		 <publisher>JACoW</publisher>
       <pub-location>Geneva, Switzerland</pub-location>
		 <isbn>978-3-95450-167-0</isbn>
		 <electronic-resource-num>10.18429/JACoW-Cyclotrons2016-WEB04</electronic-resource-num>
		 <language>English</language>
		 <pages>270-273</pages>
       <pages>WEB04</pages>
       <keywords>
          <keyword>cyclotron</keyword>
          <keyword>ion</keyword>
          <keyword>injection</keyword>
          <keyword>extraction</keyword>
          <keyword>acceleration</keyword>
       </keywords>
       <work-type>Contribution to a conference proceedings</work-type>
       <dates>
          <year>2017</year>
          <pub-dates>
             <date>2017-01</date>
          </pub-dates>
       </dates>
       <urls>
          <related-urls>
              <url>http://dx.doi.org/10.18429/JACoW-Cyclotrons2016-WEB04</url>
              <url>http://jacow.org/cyclotrons2016/papers/web04.pdf</url>
          </related-urls>
       </urls>
       <abstract>
          A concept of coupled cyclotrons for acceleration of carbon ions (charge 6+) to 400 MeV/nucleon by a separated sector cyclotron consisting of six sector magnets with superconducting coils is proposed. Injection to the machine will be provided by a compact 70 MeV/nucleon cyclotron. The accelerator complex is intended for setting up a radiation therapy facility employing carbon ions. The advantages of the dual cyclotron design are typical of cyclotron-based solutions. The first design studies of the sector magnet of the main cyclotron (magnetic field increases from 4.2 T to 6.5 T, RF frequency 73.56 MHz, RF mode 6) show that it is feasible with acceptable beam dynamics. The accelerator has a relatively compact size (outer diameter of 8 m) and can be an alternative to synchrotrons.
       </abstract>
    </record>
  </records>
</xml>
